Quarkonium results in pa & AA: from RHIC to LHC
|
|
- Delphia Bryant
- 6 years ago
- Views:
Transcription
1 International School of Nuclear Physics 38 th course Nuclear matter under extreme conditions relativistic heavy-ion collisions September 2016 Quarkonium results in pa & AA: from RHIC to LHC Roberta Arnaldi INFN Torino
2 International School of Nuclear Physics 38 th course Nuclear matter under extreme conditions relativistic heavy-ion collisions September 2016 Outlook: Selection on results on Charmonium: J/ and (2S) Bottomonium: (1S), (2S), (3S) in p-a, d-a and A-A collisions at RHIC and LHC energies
3 J/ production probability AA: hot matter effects 3 the original idea quarkonium production suppressed via color screening in the QGP sequential melting differences in quarkonium binding energies lead to a sequential melting with increasing temperature T.Matsui and H.Satz, Phys.Lett.B178 (1986) 416 Statistical regeneration (re)combination enhanced quarkonium production through (re)combination during QGP phase or at hadronization Central AA collisions SPS 20 GeV RHIC 200 GeV LHC 2.76TeV LHC 5.02TeV N ccbar /event ~0.2 ~10 ~85 ~115 Sequential melting energy density P. Braun-Muzinger,J. Stachel, PLB 490(2000) 196 R. Thews et al, Phys.Rev.C63:054905(2001)
4 pa: CNM effects 4 Cold nuclear matter effects: might affect quarkonium production on top of hot matter mechanisms nuclear parton shadowing/ color glass condensate energy loss c c in medium break-up investigated in p-a collisions the assessment of the size of these effects is fundamental to interpret quarkonium A-A results Nuclear modification factor J ψ R AA = J ψ Y AA J ψ T AA σ pp Medium effects are quantified comparing the AA quarkonium yield with the pp one, scaled by a geometrical factor (from Glauber model) R AA = 1 no medium effects R AA 1 hot/cold matter effects
5 Quarkonium in HI 5 p-a p-p vacuum reference for A-A and p-a, genuine pp physics program cold nuclear warm/hot matter effects: matter shadowing/cgc, effects? hadronic energy loss resonance gas (comovers), partonic matter hot matter effects: regeneration vs suppression A-A
6 Quarkonium at RHIC & LHC 6 Facility Experiment System s NN (GeV) RHIC LHC PHENIX STAR ALICE ATLAS CMS LHCb Au-Au, Cu-Cu, Cu-Au, U-U 200, 193, 62, 39 p-a, d-au 200 pp Pb-Pb p-pb 5020 (8000) pp 2760, 7000, 8000, Data taking (2016)
7 Quarkonium at RHIC & LHC 7 Facility Experiment System s NN (GeV) RHIC LHC PHENIX STAR ALICE ATLAS CMS LHCb Au-Au, Cu-Cu, Cu-Au, U-U 200, 193, 62, 39 p-a, d-au 200 pp Pb-Pb Quarkonium p-pb production 5020 investigated via collisions: (8000) with ppdifferent beam 2760, species 7000, at various energies 8000, Data taking (2016)
8 p T (GeV/c) Quarkonium at RHIC & LHC Facility Experiment System s NN (GeV) RHIC LHC PHENIX STAR ALICE ATLAS CMS LHCb Au-Au, Cu-Cu, Cu-Au, U-U 200, 193, 62, 39 Data taking p-a, d-au 200 All pp LHC experiments investigate quarkonium production Pb-Pb p-pb 5020 (8000) pp 2760, complementary 7000, results due to 8000, different kinematic coverages (2016) ATLAS J/ CMS ALICE LHCb ALICE y
9 Quarkonium at RHIC & LHC 9 Facility Experiment System s NN (GeV) RHIC LHC PHENIX STAR LHC Run-1 LHC Run-2 ALICE ATLAS CMS LHCb Au-Au, Cu-Cu, Cu-Au, U-U 200, 193, 62, 39 p-a, d-au 200 pp Pb-Pb p-pb 5020 (8000) 2760 pp 2760, , 8000, Data taking (2016)
10 Quarkonium in AA collisions 10
11 J/ suppression at RHIC 11 Stronger J/ suppression at forward-y wrt mid-y in PHENIX STAR PHENIX mid-y forward-y A. Adare et al. (PHENIX) PRC84(2011) Strong centrality and low-p T suppression Qualitative agreements with suppression + recombination models
12 Energy scan at RHIC 12 STAR PHENIX A. Adamczyk et al. (STAR) arxiv: A. Adare et al. (PHENIX) PRC86(2012) R AA suppression visible at all energies No significant energy dependence, including SPS! Qualitative agreements with suppression + recombination models pp reference at 39 & 62.4 GeV needed for quantitative comparison
13 System scan at RHIC 13 Various systems studied: rather similar suppression observed hint for a weaker suppression in U-U in central U-U collisions: PHENIX PHENIX PRC93(2016) ) stronger color screening suppression AuAu ~ 80-85% UU 2) J/ recombination favoured by 25% larger N coll in U-U N J stat ψ ~ N 2 2 c ~ N coll STAR arxiv: STAR Dominant recombination in U-U over suppression? Quantitative conclusions depend on U Woods-Saxon description
14 J/ : LHC Run1 results 14 Evidence of recombination for low p T J/ at LHC Observation validated by the comparison of LHC results with ALICE 1) lower energy experiments PHENIX forward-y ALICE Coll. PLB 734 (2014) 314 J/ suppression vs centrality is stronger in PHENIX/STAR than in ALICE, in spite of the LHC larger energy densities ALICE PHENIX, STAR Roberta Arnaldi International School of Nuclear mid-yphysics September 17 th 2016
15 J/ : LHC Run1 results Evidence of recombination for low p T J/ at LHC 15 ALICE Coll. PLB 734 (2014) 314 Observation validated by the comparison of LHC results with 1) lower energy experiments forward-y PHENIX ALICE weaker suppression at low p T observed by ALICE ALICE STAR Roberta Arnaldi International School of Nuclear mid-y Physics September 17 th 2016
16 J/ : LHC Run1 results 16 Evidence of recombination for low p T J/ at LHC Observation validated by the comparison of LHC results with ALICE 1) lower energy experiments 2) theoretical models models including (re)combination of J/ in QGP or in the hadronic phase provide a reasonable description of ALICE results still rather large theory uncertainties: models will benefit from a precise measurement of cc and CNM effects PHENIX ALICE JHEP 05 (2016) 179
17 J/ : LHC Run1 results 17 Evidence of recombination for low p T J/ at LHC Observation validated by the comparison of LHC results with 1) lower energy experiments 2) theoretical models 3) high p T J/ results suppression stronger at higher s, as expected from QGP dissociation CMS STAR opposite J/ behavior compared to low-p T results negligible re(combination) effects expected at high p T
18 J/ flow 18 If c quarks participate to QGP collective motion, they should acquire elliptic flow J/ from (re)combination should inherit the flow of c quarks STAR, PRL (2013) ALICE, PRL 111(2013) CMS-PAS-HIN ALICE CMS STAR Hint for J/ flow at LHC, contrary to v 2 ~0 observed at RHIC! ALICE: qualitative agreement with transport models including regeneration CMS: path-length dependence of energy loss?
19 J/ results from LHC Run-2 LHC: Pb-Pb s NN =5.02TeV TeV 2.76TeV arxiv:
20 J/ results from LHC Run-2 LHC: Pb-Pb s NN =5.02TeV High statistics Run-2 allows the R AA evaluation in narrow centrality bins TeV 5.02TeV 2.76TeV Similar centrality dependence at the two energies, with an increasing suppression up to N part ~100, followed by a plateau R 5.02TeV is ~15% higher than the one at 2.76TeV, even if within uncertainties arxiv:
21 J/ theory models s NN =2.76TeV s NN =5.02TeV 21 Brackets represents the possible range of variation of the hadronic J/ Comparison of same theory models at the two energies: TM1, TM2 (Du et al, Zhou et al): rate equation of suppression/regeneration in QGP SHM (Andronic et al): J/ produced by stat. hadronization at phase boundary CIM (Ferreiro): suppression by the comoving partonic medium and regeneration Data are compatible with theory models at both energies Still large uncertainties mainly due to the choice of cc
22 Run-2 J/ results 22 Theoretical and experimental uncertainties reduced in the R AA double ratio Centrality dependence of the R AA ratio is rather flat R AA increases with p T, at both energies, as expected in a regeneration scenario Hint for an increase of R AA, at 5.02TeV, in 2<p T <6 GeV/c Also s NN =5.02TeV results support a picture where a combination of J/ suppression and (re)combination occurs in the QGP
23 (2S) in AA collisions (2S) production modified in AA with a strong kinematic dependence 23 CMS ALICE CMS, PRL 113(2014) Du and Rapp arxiv: J ψ ψ(2s) < RAA Fw-y, 3<p T <30GeV/c R AA later (2S) regeneration, when radial flow is stronger, might explain the rise J ψ ψ(2s) Mid-y 6.5<p T <30GeV/c R AA > RAA stronger suppression of (2S) wrt J/ Chen et al. PLB726(2013)725 J ψ ψ(2s) Fw-y, 0<p T <3GeV/c R AA > RAA ALICE trend agrees with transport models and stat. hadronization approach JHEP 05 (2016) 179 Run1 data not precise enough to conclude on (2S) behavior Run2 results eagerly awaited!
24 (ns) production in AA 24 PRL 109, (2012) Main features of bottomonium production wrt charmonium: no B hadron feed-down smaller gluon shadowing effects negligible (re)combination more robust theoretical predictions due to the higher b quark mass with a drawback smaller production cross-section PbPb pp Clear suppression of states in PbPb at LHC energies with respect to pp collisions
25 Run-1 (ns): where we stand? Sequential suppression observed at LHC in Run 1: Υ(3S) Υ(2S) Υ(1S) R AA < RAA < RAA R AA ( (1S))= R AA ( (2S))= R AA ( (3S))< 0.14 at 95% CL centrality dependent suppression for (1S) and (2S) 25 at LHC (1S) is already suppressed in semiperipheral collisions, while at RHIC only in the central ones CMS, PRL109 (2012) and HIN STAR, PLB735 (2014) 127 and preliminary U+U feed-down from excited states + CNM are enough to explain the observed (1S) suppression?
26 LHC Run-1 (ns) results 26 no p T or y dependence of the (1S) and (2S) suppressions models reproduce the p T and centrality dependence rapidity description still needs tuning
27 LHC Run-2 (ns) results TeV 2.76TeV Centrality dependent (1S) R AA suppression observed also at s NN =5.02TeV No firm conclusion on the R AA energy dependence within the current uncertainties
28 (ns) theory models 28 Theory models, with (Emerick et al.) or without (Zhou et al.) regeneration component, qualitatively reproduce the data within uncertainties Different trend in data and theory for most forward-y?
29 (ns) at RHIC 29 (1S) is also suppressed at RHIC, in central collisions, even if less wrt LHC R AA ( (1S))= (AuAu+UU) STAR: excited states accessible in the muon channel arxiv: Hint of less suppression of excited states wrt LHC
30 Quarkonium in p-a collisions 30
31 pa J/ results at LHC 31 J/ affected by CNM effects, with a strong y and p T dependence: R pa decreases towards forward y data consistent with shadowing and coherent parton energy loss models agreement with CGC depends on implementation JHEP 02(2014)073, JHEP 06(2015)055 good agreement between ALICE and LHCb (similar kinematic range) different behavior at mid-y for low and high p T J. JHEP 02 (2014) 072 JHEP 02(2014)072
32 transv. momentum centrality J/ vs pt and centrality backward-y mid-y forward-y 32 mid and fw-y: suppression increases vs centrality and is larger at low p T backward-y: hint for increasing Q pa vs centrality, with rather flat p T trend Shadowing and coherent energy loss models in fair agreement with data
33 From pa to AA 33 Once CNM effects are measured in ppb, what can we learn on J/ production in PbPb? Hypothesis: 2 1 kinematics for J/ production CNM effects (dominated by shadowing) factorize in p-a CNM obtained as R pa x R Ap, similar x-coverage as PbPb we get rid of CNM effects with AA / pa x Ap ppb x Pbp PbPb CNM effects not enough to explain PbPb data at high p T Pb-Pb p-pb Evidence for hot matter effects in Pb-Pb!
34 (2S) production in pa, da 34 (2S) suppression is stronger than the J/ one, both at RHIC and LHC unexpected since time spent by the cc in the nucleus ( c ) is shorter than charmonium formation time ( f ) shadowing and energy loss, almost identical for J/ and (2S), do not account for the different suppression Only models including QGP + hadron resonance gas or comovers describe the stronger (2S) suppression ALICE, JHEP 1606(2016)050
35 (1s) in pa collisions 35 No significant rapidity dependence of (1S) R pa (ALICE and LHCb agree within uncertainties) Shadowing and energy loss models are compatible at forward-y At backward-y smaller antishadowing is suggested ALICE, Phys. Lett. B 740 (2015) 105 ATLAS-CONF ,LHCb, JHEP 07(2014)094
36 excited states in pa 36 p-pb vs Stronger excited states suppression with respect to (1S) Initial state effects similar for the three states Final states effects in p-pb? CMS,JHEP04(2014)103 p-pb vs : even stronger suppression of excited states in PbPb ALICE (and LHCb) observes: (2S)/ (1S) (ALICE) CMS 2.03<y<3.53: HIN , JHEP ±0.08±0.04 (2014) 103, PRL 109 (2012) -4.46<y<-2.96: 0.26±0.09±0.04 compatible with pp results 0.26 ± 0.08 (ALICE, pp@7tev) Rapidity dependent final state effects at play?
37 RHIC and LHC Prospects 37 sphenix (>2020) Precision spettroscopy (80MeV resolution expected) LHC heavy-ion program 2016: pa at s NN = 5.02 and 8 TeV 2018: PbPb : LHC Run3 L int > 10nb -1 for PbPb (is ~1nb -1 in Run2) : LHC Run4 LHCb Joined the PbPb data taking in 2015: covers peripheral semi-periph. Range SMOG: fixed target pa program at LHC, up to s =110 GeV
38 Conclusions 38 A large sample of quarkonium results in various systems and at various energies is now available from both RHIC and LHC! A combination of suppression and regeneration mechanisms affects J/ production at RHIC and LHC Theory models qualitatively describe the data, but still large uncertainties (open charm cross section) CNM effects (mainly shadowing and energy loss) play an important role, as observed in pa collisions Bottomonium results might be compatible with sequential suppression in QGP Thanks!
39 Conclusions 38 A large sample of quarkonium results in various systems and at various energies is now available from both RHIC and LHC! J/ suppression at RHIC and LHC is interpreted as a combination of suppression and regeneration mechanisms Theory models qualitatively describe the data, but still large uncertainties (open charm cross section) CNM effects (mainly shadowing and energy loss) play an important role, as observed in pa collisions Bottomonium results might be compatible with sequential suppression in QGP Thanks!
40 Backup slides 40
41 AA: from suppression the original idea: quarkonium production suppressed via color screening in the QGP 41 sequential melting differences in the quarkonium binding energies lead to a sequential melting with increasing temperature (2S) J/ (1S) T c PHENIX, Phys.Rev C91, Quarkonium as QGP thermometer T>>T c Roberta Arnaldi CONF12 August 30 th 2016
42 Evolution of J/ <p T2 > 42 ALICE,arXiv: r AA = p T 2 AA p T 2 pp r AA centrality evolution strongly depends on s decreasing r AA trend, observed at LHC due to (re)combination, which dominates J/ production at low p T TM1: Zhao et al., Nucl.Phys.A859 (2011) 114 TM2: Zhou et al. Phys.Rev.C89 (2014) transport models, already describing J/ R AA, also reproduce the r AA evolution Roberta Arnaldi CONF12 August 30 th 2016
43 J/ at very low p T Strong R AA enhancement in peripheral collisions for 0<p T <0.3 GeV/c 43 significance of the excess is 5.4 (3.4) in 70-90% (50-70%) behaviour not predicted by transport models excess might be due to coherent J/ photoproduction in PbPb (as measured also in UPC) if excess is removed requiring p T J ψ >0.3GeV/c ALICE R AA lowers by 20% at maximum (in the most peripheral bin) Roberta Arnaldi CONF12 August 30 th 2016
44 2.76TeV RAA vs pt 44 ALICE, PLB 734 (2014) 314, JHEP 07(2015)051, arxiv: TeV PHENIX Rapp Zhuang PHENIX Roberta Arnaldi CONF12 August 30 th 2016
45 Multi-differential J/ studies45 p T -centrality multi-differential studies allows detailed comparison with theory models 0-20% 20-40% 40-90% Zhao et al., Nucl.Phys.A859 (2011) 114 Zhou et al. Phys.Rev.C89 (2014) ALICE, arxiv: Model provide a fair description of the data, even if with different balance of primordial/regeneration components Still rather large theory uncertainties: models will benefit from precise measurement of cc and CNM effects Roberta Arnaldi CONF12 August 30 th 2016
46 LHC Run-2 J/ results 46 Roberta Arnaldi CONF12 August 30 th 2016
47 (2S) production in pa 47 Being more weakly bound than the J/, the (2S) is an interesting probe to have further insight on the charmonium behaviour in pa Low energy (2S) p-a results from NA50, E866 and HERA-B: mid-y (x F ~0): (2S) suppression stronger than J/ one, interpreted via pair break-up fully formed resonances traversing the nucleus E866 Collab., PRL 84 (2000) 3256 c c (2S) charmonium formation time<crossing time forward-y (high x F ): suppression becomes identical dominated by energy loss c c (2S) charmonium formation time>crossing time x F Roberta Arnaldi CONF12 August 30 th 2016
48 (2S) versus crossing time 48 c = L β z γ D. McGlinchey, A. Frawley and R.Vogt, PRC 87, (2013) Forward-y: c << f interaction with nuclear matter cannot play a role c c (2S) Backward-y: c f indication of effects related to break-up in the nucleus? c c (2S) Roberta Arnaldi CONF12 August 30 th 2016
49 (2S) / J/ double ratio 49 Similar suppression trend observed versus centrality, by both ALICE and PHENIX QGP+hadron resonance gas (Rapp) or comovers models (Ferreiro) describe the observed suppression Roberta Arnaldi CONF12 August 30 th 2016
50 Y vs ev. activity 50 CMS 50
51 Y compared to theory 51
52 J/ production at RHIC 52 (re)combination/suppression role investigated comparing U-U and AuAu in central U-U collisions: 1) stronger suppression due to color screening AuAu ~ 80-85% UU N coll scaling 2 N coll scaling 2) J/ recombination favoured by 25% larger N coll in UU 2 N J ψ stat ~ N c 2 ~ N coll 2 results slightly favour N coll scaling dominant (re)combination over suppression when going from central U-U to Au-Au collisions quantitative comparison depends on the choice of the uranium Woods-Saxon parametrizations PHENIX, arxiv: Roberta Arnaldi Quark Matter 2015 October 2 nd 2015
53 STAR CMS CMS-PAS-HIN
54 (2S) production in pa 54 (2S) suppression is stronger than the J/ one, both at RHIC and LHC unexpected since time spent by the cc in the nucleus ( c ) is shorter than charmonium formation time ( f ) shadowing and energy loss, almost identical for J/ and (2S), do not account for the different suppression Only models including QGP + hadron resonance gas or comovers describe the stronger (2S) suppression ALICE, JHEP 1606(2016)050
55 Comparison to theoretical models 55 QGP+hadron resonance gas (Rapp) or comovers models (Ferreiro) reasonably describe both J/ and (2S) suppression at RHIC and LHC pa RHIC pa LHC dau RHIC Ferreiro, PLB 749(2015)98 dau RHIC Du et al. arxiv:
56 CNM effects at RHIC 56 Disentangling CNM mechanisms is challenging shadowing + cc break-up describe R dau vs y, but meets some difficulties for R dau vs p T coherent energy loss contribution induces a less flat R dau dependence on p T -2.2<y<-1.2 Arleo et al. JHEP1305 (2013) 155
57 CNM effects at RHIC 57 Comparison between heavy flavor and quarkonium: d+au 200 GeV R da of HF muon and J/ψ are consistent at forward rapidity, but clearly different at backward rapidity charm production is enhanced but J/ψ production is significantly suppressed due to nuclear breakup inside dense comovers at backward rapidity Contrarily to LHC, at RHIC energies a contribution from J/ breakup in nuclear matter could be present ( J/ -N ~ 4mb) PHENIX: PRC PHENIX: PRL
Quarkonium production in proton-nucleus collisions
INT Program INT-17-1b Precision spectroscopy of QGP properties with jets and heavy quarks May 31 st 2017 Quarkonium production in proton-nucleus collisions Roberta Arnaldi INFN Torino INT Program INT-17-1b
More informationQuarkonium results: lessons from LHC run-1
Quarkonium results: lessons from LHC run-1 E. Scomparin (INFN-Torino) Trento, March 16-20 2015 Introduction, pre-lhc summary LHC run-1 substantial progress on charmonium/bottomonium studies! Open points
More informationQuarkonium production at LHC: from pp to AA
Quarkonium production at LHC: from pp to AA E. Scomparin (INFN-Torino) A short introduction Building on the shoulders of giants LHC results New discoveries, better understanding Open points and prospects
More informationOverview of Quarkonium Production in Heavy-Ion Collisions at LHC
XLV International Symposium on Multiparticle Dynamics (ISMD2015) Wildbad Kreuth, Germany, October 4-9, 2015 Overview of Quarkonium Production in Heavy-Ion Collisions at LHC Byungsik Hong (Korea University)
More informationOutlook: 1) Hard probes: definitions. 2) High p T hadrons. 3) Heavy Flavours
5 th International School on QGP and Heavy Ions Collisions: past, present and future Torino, 5-12 March 2011 1 Outlook: 1) Hard probes: definitions 2) High p T hadrons 3) Heavy Flavours 4) Quarkonia 1)
More informationRoberta Arnaldi INFN, Torino for the ALICE Collaboration. Quarkonia in deconfined matter Acitrezza, September 28 th -30 th
Roberta Arnaldi INFN, Torino for the ALICE Collaboration Quarkonia in deconfined matter Acitrezza, September 28 th -30 th 2011 1 Physics motivations J/ψ measurement in PbPb collisions @ 2.76 TeV with ALICE
More informationHeavy-ion collisions in a fixed target mode at the LHC beams
Heavy-ion collisions in a fixed target mode at the LHC beams Alexey Kurepin 1, and Nataliya Topilskaya 1, 1 Institute for Nuclear Research, RAS, Moscow, Russia Abstract. The interaction of high-energy
More informationCharmonium production in heavy ion collisions.
Charmonium production in heavy ion collisions. N.S.Topilskaya and A.B.Kurepin INR RAS, Moscow 1. Physical motivaion. 2. Experimental situation. 3. Fixed target suggestion. 3. Summary. N.S.Topilskaya, ISHEPP
More informationQuarkonia physics in Heavy Ion Collisions. Hugo Pereira Da Costa CEA/IRFU Rencontres LHC France Friday, April
Quarkonia physics in Heavy Ion Collisions Hugo Pereira Da Costa CEA/IRFU Rencontres LHC France Friday, April 5 2013 1 2 Contents Introduction (QGP, Heavy Ion Collisions, Quarkonia) Quarkonia at the SPS
More informationHeavy Flavours in ALICE
Heavy Flavours in ALICE Yvonne Pachmayer, University of Heidelberg for the ALICE Collaboration Motivation Cold nuclear matter effects Results from p-pb collisions Open heavy flavour J/ψ, ψ(2s), ϒ(1S) Comparison
More informationLatest results on Quarkonium production in nuclear matter at the LHC
Latest results on Quarkonium production in nuclear matter at the LHC Nicolas Filipovic ELTE Particle Physics Seminar April 27th, 2016 Outline A Quarkonium in the QGP Charmonium results in Run 1 Bottomonium
More informationQuarkonium production measurement in Pb-Pb collisions at forward and mid rapidity with the ALICE experiment
Quarkonium production measurement in Pb-Pb collisions at forward and mid rapidity with the ALICE experiment Lizardo Valencia Palomo Institut de Physique Nucléaire d Orsay (CNRS-IN2P3, Université Paris-Sud
More informationHeavy quarks: where do we stand? What next?
Heavy quarks: where do we stand? What next? E. Scomparin (INFN-Torino) Student Day, May 18, 2014 Quarkonia Sensitive to the temperature of QGP c c Color Screening Probe the opacity of QGP Open heavy quarks
More informationarxiv: v2 [hep-ex] 9 Oct 2014
J/ψ and ψ(2s) production in p-pb collisions with ALICE at the LHC arxiv:1410.1761v2 [hep-ex] 9 Oct 2014 for the ALICE Collaboration INFN and University, Torino E-mail: leoncino@to.infn.it The ALICE collaboration
More informationBeijing. Charmed hadron signals of partonic medium. Olena Linnyk
Beijing Charmed hadron signals of partonic medium Olena Linnyk Our goal properties of partonic matter Hadron-string models Experiment QGP models Observables Hadron abundances J/Ψ anomalous suppression
More informationOverview of recent ALICE results
Overview of recent ALICE results E. Scomparin (INFN-Torino) A short introduction Heavy ions at the LHC The ALICE experiment Characterization of the QGP The physics program Global observables The most liquid
More informationarxiv: v1 [nucl-ex] 7 Jan 2019
Open Heavy Flavour: Experimental summary arxiv:9.95v [nucl-ex] 7 Jan 9 Deepa homas he University of exas at Austin E-mail: deepa.thomas@cern.ch In this paper I will review a few of the latest experimental
More informationQuarkonia and heavy-quark production in proton and nuclear collisions at the LHC
Quarkonia and heavy-quark production in proton and nuclear collisions at the LHC Michael Schmelling / MPI for Nuclear Physics Introduction Double Parton Scattering Cold Nuclear Matter Effects Quark Gluon
More informationResults on heavy ion collisions at LHCb
Results on heavy ion collisions at LHCb Marcin Kucharczyk on behalf of LHCb collaboration HNI Krakow 28th Rencontres de Blois 29.05-03.06 2016 Outline LHCb - general purpose forward experiment Physics
More informationResults with Hard Probes High p T Particle & Jet Suppression from RHIC to LHC
Results with Hard Probes High p T Particle & Jet Suppression from RHIC to LHC PHENIX! AGS! RHIC! STAR! Cover 3 decades of energy in center-of-mass s NN = 2.76 TeV 5.5 TeV (2015) CMS LHC! s NN = 5-200 GeV
More informationHidden heavy flavour production in heavy-ion collisions
Hidden heavy flavour production in heavyion collisions Javier Castillo Castellanos 1, 1 IRFU, CEA, Université ParisSaclay, F91191GifsurYvette, France Abstract. An overview of recent experimental results
More informationHeavy Flavor Results from STAR
Heavy Flavor Results from STAR Wei Xie for STAR Collaboration (PURDUE University, West Lafayette) Open Heavy Flavor Production D meson direct measurement Non-photonic electron Heavy Quarkonia Production
More informationJ/ suppression in relativistic heavy-ion collisions
J/ suppression in relativistic heavy-ion collisions Partha Pratim Bhaduri VECC, Kolkata 61st DAE-BRNS SYMPOSIUM ON NUCLEAR PHYSICS SAHA INSTITUTE OF NUCLEAR PHYSICS Kolkata, India Challenge: find the good
More informationUltra-Relativistic Heavy Ion Collision Results
Ultra-Relativistic Heavy Ion Collision Results I. Overview of Effects Observed in Large Nucleus-Nucleus Collision Systems (Au+Au, Pb+Pb) High p T Hadrons Are Suppressed at LHC & RHIC Central Pb-Pb and
More informationCharm production at RHIC
1 Charm production at RHIC Charm 2007 Conference Cornell University, Ithaca, NY 5 August 2007 2 The Quark Gluon Plasma T c Early universe quark-gluon plasma LHC RHIC Tri-critical point? Quark deconfinement
More informationHeavy flavour production at RHIC and LHC
Heavy flavour production at RHIC and LHC Gian Michele Innocenti 1, 1 Massachusetts Institute of Technology Abstract. In this proceedings, I present selected experimental results on heavy-flavour production
More informationExperimental Overview on Heavy Flavor Production in Heavy Ion Collisions.
Experimental Overview on Heavy Flavor Production in Heavy Ion Collisions. Cesar L. da Silva 1, 1 Los Alamos National Lab - USA Abstract. The use of probes containing heavy quarks is one of the pillars
More informationLHCb results in proton-nucleus collisions at the LHC
LHCb results in proton-nucleus collisions at the LHC PANIC August 28, 2014 on behalf of the LHCb collaboration Outline Motivation LHCb Detector Beam configurations Measurements J/Ψ production Υ production
More informationConference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
Available on the CMS information server CMS CR 3-78 he Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH- GENEVA 3, Switzerland 8//9 Υ suppression in PbPb collisions at the
More informationFirst results with heavy-ion collisions at the LHC with ALICE
First results with heavy-ion collisions at the LHC with ALICE Domenico Elia INFN, Bari (Italy) on behalf of the ALICE Collaboration D. Elia (INFN Bari, Italy) PANIC 011 / Boston, MA (USA) July 4-9, 011
More informationOverview of heavy ion CMS results
Overview of heavy ion CMS results Gian Michele Innocenti on behalf of the CMS Collaboration Massachusetts Institute of echnology Rencontres de Moriond QCD and High Energy Interactions March 19th - 26th,
More informationReview of photon physics results at Quark Matter 2012
Review of photon physics results at Quark Matter 2012 Jet Gustavo Conesa Balbastre 1/28 Why photons? Direct thermal: Produced by the QGP Measure medium temperature R AA > 1, v 2 > 0 Direct prompt: QCD
More informationRAA and v2 of muons from heavy quark decays in 2.76 TeV data with ATLAS
RAA and v2 of muons from heavy quark decays in 2.76 TeV data with ATLAS Alexander Milov For the ATLAS CollaboraEon Data sample summary Year Species s NN [TeV] L int [nb - 1 ] Triggers 2010 Pb+Pb 2.76 0.01
More informationRecent results from relativistic heavy ion collisions
Recent results from relativistic heavy ion collisions Camelia Mironov MI at the LHC A teaser talk with very few (though recent) results LHC Heavy-Ion (HI) Program Collision systems Center of mass colliding
More informationRecent Quarkonia results by PHENIX
Recent Quarkonia results by PHENIX Disclaimer: this is not a review of all the results Zaida Conesa del Valle Laboratoire Leprince-Ringuet Rencontres de Moriond, March 2009 The historical introduction,
More information+ High p T with ATLAS and CMS in Heavy-Ion 2.76TeV
+ High p T with ATLAS and CMS in Heavy-Ion Collisions @ 2.76TeV Lamia Benhabib On behalf of ATLAS and CMS HCP 2011, Paris lamia.benhabib@llr.in2p3.fr +Outlook Introduction : hard probes Strongly interacting
More informationMeasurement of quarkonium production at the LHC: from pp to Pb Pb collisions with insight into the Quark-Gluon Plasma
Measurement of quarkonium production at the LHC: from pp to Pb Pb collisions with insight into the Quark-Gluon Plasma A. Andronic GSI Darmstadt Quarkonium production in pp and p Pb collisions Quarkonium
More informationarxiv: v1 [hep-ex] 14 Jan 2016
Nuclear Physics A Nuclear Physics A (28) 5 www.elsevier.com/locate/procedia arxiv:6.352v [hep-ex] 4 Jan 26 Measurements of heavy-flavour nuclear modification factor and elliptic flow in Pb Pb collisions
More informationLHCb results from proton-ion collisions
LHCb results from proton-ion collisions L. Massacrier on behalf of the LHCb collaboration Laboratoire de l Accélérateur Linéaire, Orsay Institut de Physique Nucléaire d Orsay XLV International Symposium
More informationarxiv: v1 [nucl-ex] 29 Sep 2014
Inclusive J/ψ and ψ(s) production in and p-pb collisions at forward rapidit with ALICE at the LHC arxiv:49.877v [nucl-ex] 9 Sep 4 Biswarup Paul (for the ALICE Collaboration) Saha Institute of Nuclear Phsics,
More informationProduction of Charmed Hadrons by Statistical Hadronization of a Quark Gluon Plasma as a proof of deconfinement
Production of Charmed Hadrons by Statistical Hadronization of a Quark Gluon Plasma as a proof of deconfinement statistical hadronization model comparison to RHIC data (also SPS) predictions for LHC comments
More informationStatus of Heavy-Ion Physics at the LHC
Status of Heavy-Ion Physics at the LHC Yvonne Pachmayer, Heidelberg University J. Jowett LHC Page 1 2 Motivation: What is the question? ALICE/LHC Pb+Pb snn = 2760 GeV What happens if you make matter Hotter
More informationQuarkonium production in CMS
Quarkonium production in CMS Hyunchul Kim (Korea University For the CMS collaboration Content CMS detector@lhc Quarkonia physics motivation Result from CMS Charmonia : J/ψ Bottomonia : ϒ Summary HIM@Pyeongchang,
More informationALICE results in p Pb collisions at the LHC
ALICE results in p Pb collisions at the LHC Diego Stocco for the ALICE Collaboration (Ecole des Mines, CNRS-INP3, Université de Nantes) Nantes, France Outline Motivation Goal p Pb collisions Experimental
More informationSTAR heavy-ion highlights
STAR heavy-ion highlights Olga Rusnakova (for the STAR Collaboration) 1,a 1 Czech Technical University in Prague, Faculty of Nuclear Sciences and Physical Engineering, Brehova 7, Praha 1 Abstract. Parton
More informationExperimental summary: heavy-flavour production at the LHC
Experimental summary: heavy-flavour production at the LHC Gian Michele Innocenti Massachusetts Institute of Technology (MIT) 8th International Conference on Hard and Electromagnetic Probes of High-energy
More informationLLR, École polytechnique IN2P3/CNRS, Palaiseau, France 2. LAPTh, Université de Savoie CNRS, Annecy-le-Vieux, France 3
Color screening in Quark Gluon Plasma (QGP): A new experiment to measure charm production in PbPb collisions at the CERN SPS CHIC: Charm in Heavy Ion Collisions F. Fleuret 1, F. Arleo 2, E. G. Ferreiro
More informationCharmonium Production and the Quark Gluon Plasma
Charmonium Production and the Quark Gluon Plasma introductory remarks on charmonium and QGP discussion of time scales and open charm conservation equation remarks on 'cold nuclear matter effects' the statistical
More informationarxiv: v1 [nucl-ex] 12 May 2008
1 Highlights from PHENIX - II arxiv:0805.1636v1 [nucl-ex] 12 May 2008 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 Terry C. Awes (for the PHENIX Collaboration ) Oak
More informationOutline: Introduction
Electromagnetic radiation in hadronic interactions: from pp to AA collisions Outline: Introduction Lijuan Ruan (Brookhaven National Laboratory) Recent results on dileptons (dielectrons) Recent results
More informationannihilation of charm quarks in the plasma
Quarkonia Production suppression vs enhancement quarkonia suppression ingredients and assumptions quarkonia in the QGP confrontation with data quarkonia enhancement ingredients and assumptions annihilation
More informationConference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
CMS CR CMS Quarkonia Measurements he Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH- GENEVA 3, Switzerland /8/6 arxiv:8.577v [hep-ex] 5 Aug Quarkonia Measurements by the
More informationHeavy quark and quarkonium evolutions in heavy ion collisions
Heavy quark and quarkonium evolutions in heavy ion collisions Baoyi Chen Tianjin University & Goethe Univeristy Main Collaborators: Pengfei Zhuang, Ralf Rapp, Yunpeng Liu, Xiaojian Du, Wangmei Zha, Carsten
More informationMeasurement of Quenched Energy Flow for Dijets in PbPb collisions with CMS
Measurement of Quenched Energy Flow for Dijets in PbPb collisions with CMS For the CMS Collaboration NPA Seminar Yale, USA 15 October, 2015 Relativistic Heavy Ion Collisions Trying to answer two important
More informationarxiv: v2 [hep-ph] 29 Jun 2010
arxiv:96.377v2 [hep-ph] 29 Jun 2 Heavy Flavor Probes of Quark-Gluon Plasma A. A. Isayev Kharkov Institute of Physics and Technology, Academicheskaya Str., Kharkov, 68, Ukraine Kharkov National University,
More informationResults and Prospects for Ion Physics at LHCb
Discovery Physics at the LHC Kruger 2016 Results and Prospects for Ion Physics at LHCb Patrick Robbe, LAL Orsay, 7 December 2016, For the LHCb Collaboration Outline The LHCb experiment Results in ppb and
More informationShingo Sakai Univ. of California, Los Angeles
Shingo Sakai Univ. of California, Los Angeles Non-photonic e result in AuAu b/c separation in non-photonic electron by electron-hadron correlations @ pp Bottom production Discuss heavy flavor energy loss
More informationHeavy flavor with
Heavy flavor with CBM@FAIR Hendrik van Hees Goethe University Frankfurt and FIAS April 21, 2015 Hendrik van Hees (GU Frankfurt/FIAS) Heavy flavor with CBM@FAIR April 21, 2015 1 / 22 Outline 1 Motivation:
More informationLHCb overview. Francesco Bossù on behalf of the LHCb collaboration. Laboratoire de l Accélérateur Linéaire, Orsay
LHCb overview Francesco Bossù on behalf of the LHCb collaboration Laboratoire de l Accélérateur Linéaire, Orsay Rencontres QGP-France 16 Étretat, -13 Oct 16 LHCb detector ˆ Single arm spectrometer, fully
More informationQuarkonia and open heavy-flavour production in high multiplicity pp collisions
Quarkonia and open heavy-flavour production in high multiplicity pp collisions Sarah Porteboeuf-Houssais for the ALICE Collaboration QGP France, Etretat, 9-12 Septembre 2013 Physics motivations in the
More informationSelected highlights from RHIC
Selected highlights from RHIC Sonia Kabana Laboratoire de Physique Subatomique et des technologies associees (SUBATECH) and University of Nantes, France QGP-France workshop Etretat, France, 9-11 September
More informationRecent highlights from STAR
EPJ Web of Conferences 7, 4 (8) SQM 7 https://doi.org/.5/epjconf/874 Recent highlights from SAR Wangmei Zha, for the SAR Collaboration Department of modern physics, University of Science and echnology
More informationElena G. Ferreiro Universidade de Santiago de Compostela, Spain
EMMI workshop Quarkonia in Deconfined Matter, Acitrezza Sicily, 27 Sept 1 Oct 2011 Elena G. Ferreiro Universidade de Santiago de Compostela, Spain Work done in collaboration with F. Fleuret, J P. Lansberg,
More informationPhenomenology of prompt photon production. in p A and A A collisions
Phenomenology of prompt photon production in p A and A A collisions François Arleo LAPTH, Annecy LPT Orsay April 2011 Francois Arleo (LAPTH) Prompt γ in p A and A A collisions LPT Orsay April 2011 1 /
More informationBottomonia physics at RHIC and LHC energies
Bottomonia physics at RHIC and LHC energies Georg Wolschin Heidelberg University Institut für Theoretische Physik Philosophenweg 16 D-69120 Heidelberg ISMD_2017_Tlaxcala Topics 1. Introduction: ϒ suppression
More informationOpen heavy-flavour production in pp, p Pb and Pb Pb collisions in ALICE
Open heavy-flavour production in pp, p Pb and Pb Pb collisions in ALICE (INFN, Bologna) on behalf of the ALICE Collaboration Bormio Winter Meeting 26/01/2018 Why open heavy flavour in ALICE? Heavy-flavour
More informationLLR, École polytechnique IN2P3/CNRS, Palaiseau, France 2. LAPTh, Université de Savoie CNRS, Annecy-le-Vieux, France 3
Color screening in Quark Gluon Plasma (QGP): An experiment to measure c c suppression in PbPb collisions at the CERN SPS CHIC: Charm in Heavy Ion Collisions F. Fleuret 1, F. Arleo 2, E. G. Ferreiro 3,
More informationPhoton and neutral meson production in pp and PbPb collisions at ALICE
Photon and neutral meson production in pp and PbPb collisions at ALICE Dieter Roehrich University of Bergen, Norway for the ALICE Collaboration Nuclear collisions at the LHC Photons as a probe for the
More informationIn-Medium Energy Loss and Correlations in Pb-Pb Collisions at 2.76 TeV with ALICE
In-Medium Energy Loss and Correlations in Pb-Pb Collisions at 2.76 TeV with ALICE Jan Fiete Grosse-Oetringhaus CERN/PH for the ALICE Collaboration Heavy Ions: Experiments Confront Theory Copenhagen, 8th
More informationAn Overview of Recent Results from the ALICE Experiment
An Overview of Recent Results from the ALICE Experiment Anders Knospe on behalf of the ALICE Collaboration he University of Houston 9 December 5 A Quick Introduction to Heavy-Ion Physics and ALICE 3 QCD
More informationHeavy flavour measurements with ALICE. heavy ion collisions & QGP heavy flavours & QGP ALICE detector overview selected physics channels
Heavy flavour measurements with ALICE heavy ion collisions & QGP heavy flavours & QGP ALICE detector overview selected physics channels Philippe.Crochet@clermont.in2p3.fr Excited QCD09, Zakopane, 09/02/09
More informationALICE results on vector meson photoproduction in ultraperipheral p-pb and Pb-Pb collisions
ALICE results on vector meson photoproduction in ultraperipheral p-pb and Pb-Pb collisions Evgeny Kryshen (Petersburg Nuclear Physics Institute, Russia) for the ALICE collaboration INT workshop INT-17-65W
More informationSTAR Open Heavy Flavor Measurements
STAR Open Heavy Flavor Measurements Xin Dong Lawrence Berkeley National Laboratory Physics Goals Mass Dependence of DE Au+Au@200GeV, 0-5% Brownian motion CUJET drag fluctuations PRL 108 (2012) 022301 Diffusion
More informationConference Report Mailing address: CMS CERN, CH-1211 GENEVA 23, Switzerland
CMS CR - he Compact Muon Solenoid Experiment Conference Report Mailing address: CMS CERN, CH- GENEVA 3, Switzerland 8/5/6 Charmonium production measured in and pp collisions by CMS arxiv:7.5v [nucl-ex]
More informationPHENIX measurements of bottom and charm quark production
Journal of Physics: Conference Series PAPER OPEN ACCESS PHENIX measurements of bottom and charm quark production To cite this article: Timothy Rinn and PHENIX Collaboration 2018 J. Phys.: Conf. Ser. 1070
More informationQuarkonia and Open Heavy Flavor Results from CMS
Quarkonia and Open Heavy Flavor Results from CMS For the CMS collaboration Heavy Quark Physics in Heavy-Ion Collisions ECT*, Trento, Italy 16-20 March, 2015 Relativistic Heavy Ion Collisions Trying to
More informationLHC: Status and Highlights
EPJ Web of Conferences 9, 9 (6) DOI:.5/ epjconf/699 QCD@Work 6 ALICE @ LHC: Status and Highlights Alberica oia,, Goethe University of Frankfurt GSI Helmholzzentrum fuer Schwerionenforschung Abstract. ALICE
More informationProton-lead measurements using the ATLAS detector
Proton-lead measurements using the ATLAS detector Martin Spousta for the ATLAS Collaboration Charles University in Prague DOI: http://dx.doi.org/10.3204/desy-proc-2014-04/275 Measurements of soft and hard
More informationHeavy-flavour measurements at LHC-ALICE. Shingo Sakai
Heavy-flavour measurements at LHC-ALICE Shingo Sakai Heavy Flavour (HF) in pp, p-pb & Pb-Pb } Heavy-flavour (charm & beauty) production } Initial hard scatterings (M HF >> Λ QCD ) } pp collisions } est
More informationJet Physics with ALICE
Jet Physics with ALICE Oliver Busch for the ALICE collaboration Oliver Busch Tsukuba 2014 /03/13 1 Outline introduction results from pp jets in heavy-ion collisions results from Pb-Pb collisions jets in
More informationReport from PHENIX. Xiaochun He Georgia State University For the PHENIX Collaboration
Report from PHENIX Xiaochun He Georgia State University For the PHENIX Collaboration Outline PHENIX status New PHENIX Results Jet and π 0 Heavy flavor Direct Photon & Flow 2 PHENIX Data Taking Mission
More informationJet quenching in heavy-ion collisions at the LHC. Marta Verweij CERN
Jet quenching in heavy-ion collisions at the LHC Marta Verweij CERN EPFL Seminar May. 2, 2016 Thousands of particles are produced in one heavy ion collision Marta Verweij 2 Heavy ion collision Marta Verweij
More informationSelected highlights from the STAR experiment at RHIC
Selected highlights from the STAR experiment at RHIC Sonia Kabana for the STAR Collaboration Laboratoire de Physique Subatomique et des technologies associees (SUBATECH) and University of Nantes, France
More informationRecent Results from RHIC: On the trail of the Quark-Gluon Plasma
Recent Results from RHIC: On the trail of the Quark-Gluon Plasma Single Au+Au Collision seen by STAR@RHIC Gunther Roland Gunther Roland/MIT July 15 2003 MPI Munich 15/7/2003 Gunther Roland/MIT www.spiegel.de
More informationCharged particle production in Pb-Pb and p-pb collisions at ALICE
Journal of Physics: Conference Series OPEN ACCESS Charged particle production in Pb-Pb and p-pb collisions at To cite this article: Chiara Oppedisano and the Collaboration J. Phys.: Conf. Ser. View the
More informationFirst LHCb results from pa and Pb-Pb collisions
First LHCb results from pa and Pb-Pb collisions L. Massacrier on behalf of the LHCb collaboration Laboratoire de l Accélérateur Linéaire, Orsay Institut de Physique Nucléaire d Orsay LHCP 016 13th 18th
More informationusing photons in p A and A A collisions
Probing parton densities and energy loss processes using photons in p A and A A collisions François Arleo LAPTH, Annecy High p Probes of High Density QCD May 2011 Francois Arleo (LAPTH) Prompt γ in p A
More informationALICE results on ultraperipheral Pb+Pb and p+pb collisions
ALICE results on ultraperipheral Pb+Pb and p+pb collisions Jaroslav Adam On behalf of the ALICE Collaboration Faculty of Nuclear Sciences and Physical Engineering Czech Technical University in Prague May
More informationCharmonium suppression
Charmonium suppression from SPS to RHIC Raphaël Granier de Cassagnac LLR École polytechnique / IN2P3 PHENIX & CMS experiments Seattle, 2009, June 17 th 1/36 Introduction overview talk on experimental status
More informationScaling patterns in ATLAS & CMS quarkonium production data
Scaling patterns in ATLAS & CMS quarkonium production data Pietro Faccioli, IST and LIP, Lisbon C. Lourenço M. Araújo J. Seixas Quarkonium Working Group, November 8 th 2017 1. shapes of the p T distributions
More informationHeavy Ion Collision Measurements at the LHC Using the CMS Detector
Heavy Ion Collision Measurements at the LHC Using the CMS Detector David Krofcheck on behalf of the CMS Collaboration IAS-CERN Workshop, Singapore, March 26 th So, what happens at the LHC besides Higgs
More informationarxiv: v2 [hep-ph] 2 Nov 2015
Charmonium Production with QGP and Hadron Gas Effects at SPS and FAIR Baoyi Chen Department of Physics, Tianjin University, Tianjin 300072, China (Dated: November 28, 2015) arxiv:1510.07902v2 [hep-ph]
More informationHeavy ion physics at LHCb
J/ψ in ppb, 8 ev D in ppb, 5 ev Λ+ c in ppb, 5 ev Heavy flavour with SMOG data Conclusion Heavy ion physics at E milie Maurice on behalf of the collaboration ICFNP 25th August 217, Kolymbari, Creta August
More informationHeavy-flavour meson production at RHIC
Heavy-flavour meson production at RHIC André Mischke ERC-Starting Independent Research Group QGP - Utrecht 1 Outline Introduction - heavy-flavour production and energy loss in QCD matter Total charm production
More informationProspective of gamma hadron correlation. study in CMS experiment
Prospective of gamma hadron correlation. study in CMS experiment Yeonju Go (Korea University) for the CMS collaboration 5-6 Dec. 2014 HIM meeting Contents Physics Motivation Direct gamma-hadron correlation
More informationRelativistic Heavy Ions Collisions at PHENIX (some of) Recent results
Relativistic Heavy Ions Collisions at PHENIX (some of) Recent results Vladislav Pantuev Stony Brook University 1 Outline: 1. Jet quenching 2. Direct photons: high pt, thermal, correlations 3. J/Ψ, cold
More informationHeavy quark(onium) at LHC: the statistical hadronization case
Heavy quark(onium) at LHC: the statistical hadronization case A.Andronic GSI Darmstadt The statistical hadronization model: assumptions and inputs Charmonium: the LHC case in light of the SPS and RHIC
More informationOpen-charm and J/ψ production at the ALICE experiment
Open-charm and J/ψ production at the ALICE experiment Pietro Cortese Università del Piemonte Orientale and INFN Alessandria, Italy on behalf of the ALICE Collaboration Purdue University, Jan. 6, 2011 Pietro
More informationUltra-relativistic nuclear collisions and Production of Hot Fireballs at SPS/RHIC
Ultra-relativistic nuclear collisions and Production of Hot Fireballs at SPS/RHIC Benjamin Dönigus 03.12.2009 Seminar WS 2009/2010 Relativistische Schwerionenphysik Interface of Quark-Gluon Plasma and
More informationRecent Heavy Ion results from ATLAS experiment
Recent Heavy Ion results from ATLAS experiment Andrzej Olszewski (INP PAN Kraków) for the ATLAS Collabora@on International Nuclear Physics Conference Adelaide Convention Centre, Australia 11-16 September
More information